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Radar System Engineering

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272 ANTENNAS, SCANNERS, A.VD STABILIZA TIO.Y [SEC. 92<br />

spicuous trend toward shorter wavelengths which has characterized radar<br />

ever since its earliest development.<br />

In the course o developing and testing a new antenna, the distribution<br />

of the energy in the beam may be expressed by means of a polar<br />

diagram or antenna pattern. Figure 9.1 displays such a pattern and<br />

FIG. 9 1.—A typical antennapattern showingthe main beamof width 61and the sidelobes.<br />

shows that the beamwidth e is the full beamwidth at half power. A<br />

small amount of po’wer is unavoidably radiated in undesired directions,<br />

forming the “side lobes’) shown in this figure.<br />

92. Round and Cut Paraboloid Antemas.-One very common type<br />

of microwave radar antenna takes the form of a paraboloidal reflector 1<br />

with a source of radiation, or “antenna feed, ” at its focus. Since the<br />

wavelength of the radiation is short in comparison<br />

with the dimensions of the reflector, it<br />

/+’<br />

is profitable in an introductory discussion to<br />

regard the operation of the antenna as a problem<br />

in ray optics (Fig. 9.2). Figure 9.2 does<br />

not explain the side lobes or the beamwidth,<br />

but it does serve to emphasize the fact that<br />

the feed is always so designed as to be directive.<br />

Figure 9.3 represents an automatic record of<br />

the energy radiated at various angles from a<br />

well-designed feed, the directional power being<br />

displayed as a function of angle. It is obvious<br />

that nearly all of the energy from the feed will<br />

FIG. 9.2.—RaY diagram of a strike a properly placed paraboloid, which will<br />

paraboloid antenna.<br />

then collimate the radiation. Figure 9.4<br />

shows the radiation from an incorrectly designed feed. A correct design,<br />

used in the 3-cm band, is illustrated in Fig. 9.5, which shows two dipoles<br />

excited by the radiation field from the ~- by l-in. waveguide transmission<br />

line. The dipoles are so adjusted in length and position that their combined<br />

effect is to direct the radiation back within a cone surrounding the<br />

line without reflecting radiation into the waveguide.<br />

Equation (1) requires further comment in the case of a paraboloid<br />

reflector of which the perimeter has been so trimmed (“ cut paraboloid”)<br />

that its width and height are unequal. If the beam is pointed horizon-<br />

I The subject of paraboloid and other types of antennas is developed in Microwave<br />

Ankmno Theory and Design, Vol. 12 of this series.

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